{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:IN7BZJWZMC63YYCMVKST22CAYS","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"2cb2f4b58efa07f08482c19fd2a5623b3bab5129739f73fc240c77c948f57573","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.other","physics.app-ph","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-08-01T11:34:44Z","title_canon_sha256":"d12cd9b0a2b27dc84e24f56a12b3ab76216c596267f143ce6362d5c939c03866"},"schema_version":"1.0","source":{"id":"2608.00599","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2608.00599","created_at":"2026-08-04T00:37:59Z"},{"alias_kind":"arxiv_version","alias_value":"2608.00599v1","created_at":"2026-08-04T00:37:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.00599","created_at":"2026-08-04T00:37:59Z"},{"alias_kind":"pith_short_12","alias_value":"IN7BZJWZMC63","created_at":"2026-08-04T00:37:59Z"},{"alias_kind":"pith_short_16","alias_value":"IN7BZJWZMC63YYCM","created_at":"2026-08-04T00:37:59Z"},{"alias_kind":"pith_short_8","alias_value":"IN7BZJWZ","created_at":"2026-08-04T00:37:59Z"}],"graph_snapshots":[{"event_id":"sha256:216d159350a9c6012392c620169c2ac3d4bb29fcb2a6af75f27431c0b78069cc","target":"graph","created_at":"2026-08-04T00:37:59Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2608.00599/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We report a previously overlooked general mechanism to obtain highly efficient spin selectivity in conventional time-reversal symmetric one-dimensional systems without invoking phase decoherence. We reveal that Rashba quantum wires featuring non-collinear spin states at the Fermi level inherently possess spin-selective transport properties. We show that this spin noncollinearity can be systematically designed and engineered by introducing an additional pseudospin degree of freedom - such as valley, sublattice, or orbital angular momentum - into spin-orbit coupled systems. By applying this fram","authors_text":"Carmine Ortix, Luciano Jacopo D'Onofrio, Maria Teresa Mercaldo, Mario Cuoco","cross_cats":["cond-mat.mtrl-sci","cond-mat.other","physics.app-ph","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-08-01T11:34:44Z","title":"Spin selectivity induced by non-collinear spins in Rashba wires"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.00599","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:0805db13072a1c24babebfae0ba5121dd62bb17a6b05ea5b1653b7ac9ddb9aa8","target":"record","created_at":"2026-08-04T00:37:59Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"2cb2f4b58efa07f08482c19fd2a5623b3bab5129739f73fc240c77c948f57573","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.other","physics.app-ph","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-08-01T11:34:44Z","title_canon_sha256":"d12cd9b0a2b27dc84e24f56a12b3ab76216c596267f143ce6362d5c939c03866"},"schema_version":"1.0","source":{"id":"2608.00599","kind":"arxiv","version":1}},"canonical_sha256":"437e1ca6d960bdbc604caaa53d6840c4ad90f5e6e998abe75386899909fad8e1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"437e1ca6d960bdbc604caaa53d6840c4ad90f5e6e998abe75386899909fad8e1","first_computed_at":"2026-08-04T00:37:59.706375Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-08-04T00:37:59.706375Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rN1SOLALfLCaChnZNTr4tWoIn3UBCh+ReaWiz6Uaa/POrNfxxPEo8plCU1ArCRbmhuXvjfYfzZx83FLdKA1vDQ==","signature_status":"signed_v1","signed_at":"2026-08-04T00:37:59.707860Z","signed_message":"canonical_sha256_bytes"},"source_id":"2608.00599","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0805db13072a1c24babebfae0ba5121dd62bb17a6b05ea5b1653b7ac9ddb9aa8","sha256:216d159350a9c6012392c620169c2ac3d4bb29fcb2a6af75f27431c0b78069cc"],"state_sha256":"250a5447f392ed8a924ffeebcfbf26fa8307520d92e833e5afeb905ed32179c0"}